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Tunability of the topological nodal-line semimetal phase in ZrSi X-type materials (X = S, Se, Te)

机译:ZrSi X型材料(X = S,Se,Te)中的拓扑节点线半金属相的可调谐性

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摘要

The discovery of a topological nodal-line (TNL) semimetal phase in ZrSiS has invigorated the study of other members of this family. Here, we present a comparative electronic structure study of ZrSiX (where X = S, Se, Te) using angle-resolved photoemission spectroscopy (ARPES) and first-principles calculations. Our ARPES studies show that the overall electronic structure of ZrSiX materials comprises the diamond-shaped Fermi pocket, the nearly elliptical-shaped Fermi pocket, and a small electron pocket encircling the zone center (Γ) point, the M point, and the X point of the Brillouin zone, respectively. We also observe a small Fermi surface pocket along the M-Γ-M direction in ZrSiTe, which is absent in both ZrSiS and ZrSiSe. Furthermore, our theoretical studies show a transition from nodal-line to nodeless gapped phase by tuning the chalcogenide from S to Te in these material systems. Our findings provide direct evidence for the tunability of the TNL phase in ZrSiX material systems by adjusting the spin-orbit coupling strength via the X anion.
机译:ZrSiS中拓扑节点线(TNL)半金属相的发现激发了对该族其他成员的研究。在这里,我们使用角度分辨光发射光谱(ARPES)和第一性原理计算方法对ZrSiX(其中X = S,Se,Te)进行了比较电子结构研究。我们的ARPES研究表明,ZrSiX材料的整体电子结构包括菱形的费米腔,近乎椭圆形的费米腔以及围绕区域中心(Γ)点,M点和X点的小电子腔分别是布里渊区。我们还在ZrSiTe中沿M-Γ-M方向观察到一个小的费米表面凹穴,这在ZrSiS和ZrSiSe中均不存在。此外,我们的理论研究表明,通过在这些材料系统中将硫族化物从S转变为Te,可以从节点线过渡到无节点的间隙相。我们的发现通过调节X阴离子的自旋轨道耦合强度,为ZrSiX材料系统中TNL相的可调谐性提供了直接证据。

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  • 来源
    《Physical review. B, Condensed Matter And Materials Physics》 |2017年第16期|161101.1-161101.6|共6页
  • 作者单位

    Department of Physics, University of Central Florida, Orlando, Florida 32816, USA;

    Department of Physics, University of Central Florida, Orlando, Florida 32816, USA;

    Joseph Henry Laboratory and Department of Physics, Princeton University, Princeton, New Jersey 08544, USA;

    Department of Physics and Astronomy, Uppsala University, P.O. Box 516, S-75120 Uppsala, Sweden;

    Institute of Physics, Academia Sinica, Taipei 10617, Taiwan,Center for Condensed Matter Sciences, National Taiwan University, Taipei 10617, Taiwan;

    Department of Physics, University of Central Florida, Orlando, Florida 32816, USA;

    Department of Physics, University of Central Florida, Orlando, Florida 32816, USA;

    Department of Physics, University of Central Florida, Orlando, Florida 32816, USA;

    Department of Physics and Astronomy, Uppsala University, P.O. Box 516, S-75120 Uppsala, Sweden;

    Institute of Low Temperature and Structure Research, Polish Academy of Sciences, PL-50-950 Wroclaw, Poland;

    Center for Condensed Matter Sciences, National Taiwan University, Taipei 10617, Taiwan;

    Joseph Henry Laboratory and Department of Physics, Princeton University, Princeton, New Jersey 08544, USA;

    Condensed Matter and Magnet Science Group, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA,Institute of Physics, Maria Curie-Sklodowska University, PL-20-031 Lublin, Poland;

    Department of Physics, University of Central Florida, Orlando, Florida 32816, USA;

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